Exact Hausdorff measure of SLE boundary contacts

The dimension of a random fractal specifies its scaling exponent; a finite, nonzero measure requires a finer calibration. We determine this calibration for the boundary contacts of chordal SLEκ, 4 < κ < 8. With δ = 2 − 8/κ and β = 8/κ − 1, the exact Hausdorff gauge is h(r) = rδ[log log(1/r)]β. The associated Hausdorff measure on the entire boundary contact set equals a deterministic positive constant times the canonical boundary measure, simultaneously for all Borel sets. The exponent β is sharp: smaller iterated logarithmic powers give zero measure and larger powers give infinite measure on sets of positive finite canonical mass. The proof combines an explicit product bound for Green functions of every order with estimates uniform over the past at actual contact stopping times. An inverse boundary mass clock yields recurrence along one curve, and a covering argument removes all exceptional contacts at zero Hausdorff cost. The resulting identity recovers the canonical boundary mass, and its completed clock, directly from Euclidean geometry.

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-08
DOI
https://doi.org/10.5281/zenodo.23233356
Primary Topic
Stochastic processes and statistical mechanics
Type
preprint
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preprint

Exact Hausdorff measure of SLE boundary contacts

Zixuan He
Zenodo (CERN European Organization for Nuclear Research)
Stochastic processes and statistical mechanics
preprint

Exact Hausdorff measure of SLE boundary contacts

Zixuan He
preprint en

Abstract

The dimension of a random fractal specifies its scaling exponent; a finite, nonzero measure requires a finer calibration. We determine this calibration for the boundary contacts of chordal SLEκ, 4 < κ < 8. With δ = 2 − 8/κ and β = 8/κ − 1, the exact Hausdorff gauge is h(r) = rδ[log log(1/r)]β. The associated Hausdorff measure on the entire boundary contact set equals a deterministic positive constant times the canonical boundary measure, simultaneously for all Borel sets. The exponent β is sharp: smaller iterated logarithmic powers give zero measure and larger powers give infinite measure on sets of positive finite canonical mass. The proof combines an explicit product bound for Green functions of every order with estimates uniform over the past at actual contact stopping times. An inverse boundary mass clock yields recurrence along one curve, and a covering argument removes all exceptional contacts at zero Hausdorff cost. The resulting identity recovers the canonical boundary mass, and its completed clock, directly from Euclidean geometry.

Zenodo (CERN European Organization for Nuclear Research)
University of Glasgow (GB)
Stochastic processes and statistical mechanics
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